586 research outputs found

    Cognitive Ability and Cardiovascular Control in Intellectually and Developmentally Disabled People

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    Earlier, we examined positive effects of hyperoxic air on the cognitive ability of intellectually and developmentally disabled people (IDDP). In this study, correlation between cognitive performance in the visual matching task and heart rate (HR) was investigated under normal air conditions. Eighteen men (mean age 28.7 ± 5.0 year) and 22 women (mean age 35.5 ± 6.9 year) with an assessed disability level of 2.3 ± 0.6 participated. The experiment consisted of three phases, a total of 7 min, including the rest (3 min), control (2 min), and visual matching task 2 min phases. The HR in visual matching task phase increased, compared to those in the rest and control phases. The cognitive ability in the visual matching task correlated with the HR values; the response time showed a negative correlation with HR, while the accuracy rate showed a positive correlation. Thus, adaptive changes in cardiovascular regulation probably related to cognitive efforts and emotional excitation should be considered a noticeable factor influencing brain supply with oxygen in IDDP (similarly to healthy people). The result of this study agrees with the earlier obtained indications that hyperoxic air can positively affect the cognitive performance in IDDP.Đ Đ°ĐœŃ–ŃˆĐ” ĐŒĐž ĐČĐžĐČчалО ĐżĐŸĐ·ĐžŃ‚ĐžĐČĐœŃ– ĐČплОĐČĐž ĐżĐŸĐČітря, Đ·Đ±Đ°ĐłĐ°Ń‡Đ”ĐœĐŸĐłĐŸ ĐșĐžŃĐœĐ”ĐŒ, ĐœĐ° ĐșĐŸĐłĐœŃ–Ń‚ĐžĐČĐœŃ– Đ·ĐŽĐ°Ń‚ĐœĐŸŃŃ‚Ń– люЎДĐč Đ· ĐœĐ”ĐŽĐŸŃŃ‚Đ°Ń‚ĐœŃ–ĐŒ Ń–ĐœŃ‚Đ”Đ»Đ”ĐșŃ‚ŃƒĐ°Đ»ŃŒĐœĐžĐŒ Ń€ĐŸĐ·ĐČотĐșĐŸĐŒ (НІР). ĐŁ ĐœĐ°ŃˆŃ–Đč Ń€ĐŸĐ±ĐŸŃ‚Ń– ĐŒĐž ĐŽĐŸŃĐ»Ń–ĐŽĐ¶ŃƒĐČалО ĐșĐŸŃ€Đ”Đ»ŃŃ†Ń–ŃŽ ĐŒŃ–Đ¶ ĐżĐŸĐșĐ°Đ·ĐœĐžĐșĐ°ĐŒĐž ĐșĐŸĐłĐœŃ–Ń‚ĐžĐČĐœĐŸŃ— Đ°ĐșтоĐČĐœĐŸŃŃ‚Ń– ĐČ Ń‚Đ”ŃŃ‚Ń– ĐČŃ–Đ·ŃƒĐ°Đ»ŃŒĐœĐŸŃ— ĐČŃ–ĐŽĐżĐŸĐČŃ–ĐŽĐœĐŸŃŃ‚Ń– та Ń‡Đ°ŃŃ‚ĐŸŃ‚ĐŸŃŽ сДрцДĐČох сĐșĐŸŃ€ĐŸŃ‡Đ”ĐœŃŒ (ЧХХ) у таĐșох ŃŃƒĐ±â€™Ń”ĐșтіĐČ ĐČ ŃƒĐŒĐŸĐČах ĐŽĐžŃ…Đ°ĐœĐœŃ ĐœĐŸŃ€ĐŒĐ°Đ»ŃŒĐœĐžĐŒ ĐżĐŸĐČŃ–Ń‚Ń€ŃĐŒ. ĐŁ тДстах бралО участь 18 Ń‡ĐŸĐ»ĐŸĐČіĐșіĐČ (ŃĐ”Ń€Đ”ĐŽĐœŃ–Đč ĐČіĐș 28.7 ± 5.0 Ń€ĐŸĐșу) та 22 Đ¶Ń–ĐœĐșĐž (35.5 ± 6.9 Ń€ĐŸĐșу) Đ· ĐŸŃ†Ń–ĐœĐșĐŸŃŽ ріĐČĐœŃ Ń–ĐœŃ‚Đ”Đ»Đ”ĐșŃ‚ŃƒĐ°Đ»ŃŒĐœĐŸĐłĐŸ Ń€ĐŸĐ·ĐČотĐșу 2.3 ± 0.6. ЕĐșŃĐżĐ”Ń€ĐžĐŒĐ”ĐœŃ‚ (Đ·Đ°ĐłĐ°Đ»ŃŒĐœĐ° троĐČĐ°Đ»Ń–ŃŃ‚ŃŒ 7 хĐČ) сĐșлаЎаĐČся Đ· Ń‚Ń€ŃŒĐŸŃ… Ń„Đ°Đ·: ŃŃ‚Đ°Đœ Ń€ĐŸĐ·ŃĐ»Đ°Đ±Đ»Đ”ĐœĐœŃ (3 хĐČ), ĐșĐŸĐœŃ‚Ń€ĐŸĐ»ŃŒ (2 хĐČ) та тДст ĐČŃ–Đ·ŃƒĐ°Đ»ŃŒĐœĐŸŃ— ĐČŃ–ĐŽĐżĐŸĐČŃ–ĐŽĐœĐŸŃŃ‚Ń– (2 хĐČ). Đ’Đ”Đ»ĐžŃ‡ĐžĐœĐž ЧХХ у ĐŒĐ”Đ¶Đ°Ń… Ń†ŃŒĐŸĐłĐŸ Ń‚Đ”ŃŃ‚Ńƒ ĐżĐŸŃ€Ń–ĐČĐœŃĐœĐŸ Đ· ĐČĐ”Đ»ĐžŃ‡ĐžĐœĐ°ĐŒĐž ĐČ ŃƒĐŒĐŸĐČах Ń€ĐŸĐ·ŃĐ»Đ°Đ±Đ»Đ”ĐœĐœŃ Đč ĐșĐŸĐœŃ‚Ń€ĐŸĐ»ŃŽ Đ·Ń€ĐŸŃŃ‚Đ°Đ»Đž. ĐŸĐŸĐșĐ°Đ·ĐœĐžĐșĐž ĐșĐŸĐłĐœŃ–Ń‚ĐžĐČĐœĐžŃ… Đ·ĐŽŃ–Đ±ĐœĐŸŃŃ‚Đ”Đč ĐșĐŸŃ€Đ”Đ»ŃŽĐČалО Đ· ĐČĐ”Đ»ĐžŃ‡ĐžĐœĐ°ĐŒĐž ЧХХ; ĐșĐŸŃ€Đ”Đ»ŃŃ†Ń–Ń часу ĐČŃ–ĐŽĐżĐŸĐČіЮі була ĐœĐ”ĐłĐ°Ń‚ĐžĐČĐœĐŸŃŽ, Đ° Ń‚ĐŸŃ‡ĐœĐŸŃŃ‚Ń– ĐČŃ–ĐŽĐżĐŸĐČіЮі – ĐżĐŸĐ·ĐžŃ‚ĐžĐČĐœĐŸŃŽ. ОтжД, аЮаптоĐČĐœŃ– Đ·ĐŒŃ–ĐœĐž Ń€Đ”ĐłŃƒĐ»ŃŃ†Ń–Ń— сДрцДĐČĐŸ-ŃŃƒĐŽĐžĐœĐœĐŸŃ— ŃĐžŃŃ‚Đ”ĐŒĐž, ĐŒĐ°Đ±ŃƒŃ‚ŃŒ, ĐżĐŸĐČâ€™ŃĐ·Đ°ĐœŃ– Đ· ĐșĐŸĐłĐœŃ–Ń‚ĐžĐČĐœĐžĐŒĐž Đ·ŃƒŃĐžĐ»Đ»ŃĐŒĐž та Đ”ĐŒĐŸŃ†Ń–ĐčĐœĐžĐŒ Đ·Đ±ŃƒĐŽĐ¶Đ”ĐœĐœŃĐŒ, є Ń–ŃŃ‚ĐŸŃ‚ĐœĐžĐŒ фаĐșŃ‚ĐŸŃ€ĐŸĐŒ, яĐșĐžĐč ĐČплОĐČає ĐœĐ° ĐżĐŸŃŃ‚Đ°Ń‡Đ°ĐœĐœŃ ĐŒĐŸĐ·Đșу ĐșĐžŃĐœĐ”ĐŒ у люЎДĐč Ń–Đ· НІР (яĐș і у Đ·ĐŽĐŸŃ€ĐŸĐČох люЎДĐč). Đ Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Đž ĐœĐ°ŃˆĐŸŃ— Ń€ĐŸĐ±ĐŸŃ‚Đž ŃƒĐ·ĐłĐŸĐŽĐ¶ŃƒŃŽŃ‚ŃŒŃŃ Đ· ĐŸŃ‚Ń€ĐžĐŒĐ°ĐœĐžĐŒĐž Ń€Đ°ĐœŃ–ŃˆĐ” сĐČŃ–ĐŽĐŸŃ†Ń‚ĐČĐ°ĐŒĐž ĐżŃ€ĐŸ Ń‚Đ”, Ń‰ĐŸ ĐŽĐžŃ…Đ°ĐœĐœŃ ĐżĐŸĐČŃ–Ń‚Ń€ŃĐŒ, Đ·Đ±Đ°ĐłĐ°Ń‡Đ”ĐœĐžĐŒ ĐșĐžŃĐœĐ”ĐŒ, ĐżĐŸĐ·ĐžŃ‚ĐžĐČĐœĐŸ ĐČплОĐČає ĐœĐ° ĐșĐŸĐłĐœŃ–Ń‚ĐžĐČĐœŃ– ĐŒĐŸĐ¶Đ»ĐžĐČĐŸŃŃ‚Ń– люЎДĐč Ń–Đ· НІР

    Search for Neutral Q-balls in Super-Kamiokande II

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    A search for Q-balls induced groups of successive contained events has been carried out in Super-Kamiokande II with 541.7 days of live time. Neutral Q-balls would emit pions when colliding with nuclei, generating a signal of successive contained pion events along a track. No candidate for successive contained event groups has been found in Super-Kamiokande II, so upper limits on the possible flux of such Q-balls have been obtained.Comment: 5 pages, 5 figures, Submitted to Phys. Lett.

    Heavy Quarks and Heavy Quarkonia as Tests of Thermalization

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    We present here a brief summary of new results on heavy quarks and heavy quarkonia from the PHENIX experiment as presented at the "Quark Gluon Plasma Thermalization" Workshop in Vienna, Austria in August 2005, directly following the International Quark Matter Conference in Hungary.Comment: 8 pages, 5 figures, Quark Gluon Plasma Thermalization Workshop (Vienna August 2005) Proceeding

    Single Electrons from Heavy Flavor Decays in p+p Collisions at sqrt(s) = 200 GeV

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    The invariant differential cross section for inclusive electron production in p+p collisions at sqrt(s) = 200 GeV has been measured by the PHENIX experiment at the Relativistic Heavy Ion Collider over the transverse momentum range $0.4 <= p_T <= 5.0 GeV/c at midrapidity (eta <= 0.35). The contribution to the inclusive electron spectrum from semileptonic decays of hadrons carrying heavy flavor, i.e. charm quarks or, at high p_T, bottom quarks, is determined via three independent methods. The resulting electron spectrum from heavy flavor decays is compared to recent leading and next-to-leading order perturbative QCD calculations. The total cross section of charm quark-antiquark pair production is determined as sigma_(c c^bar) = 0.92 +/- 0.15 (stat.) +- 0.54 (sys.) mb.Comment: 329 authors, 6 pages text, 3 figures. Submitted to Phys. Rev. Lett. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.htm

    Nuclear Modification of Electron Spectra and Implications for Heavy Quark Energy Loss in Au+Au Collisions at sqrt(s_NN)=200 GeV

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    The PHENIX experiment has measured mid-rapidity transverse momentum spectra (0.4 < p_T < 5.0 GeV/c) of electrons as a function of centrality in Au+Au collisions at sqrt(s_NN)=200 GeV. Contributions from photon conversions and from light hadron decays, mainly Dalitz decays of pi^0 and eta mesons, were removed. The resulting non-photonic electron spectra are primarily due to the semi-leptonic decays of hadrons carrying heavy quarks. Nuclear modification factors were determined by comparison to non-photonic electrons in p+p collisions. A significant suppression of electrons at high p_T is observed in central Au+Au collisions, indicating substantial energy loss of heavy quarks.Comment: 330 authors, 6 pages text, 3 figures. Submitted to Phys. Rev. Lett. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.htm

    Formation of dense partonic matter in relativistic nucleus-nucleus collisions at RHIC: Experimental evaluation by the PHENIX collaboration

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    Extensive experimental data from high-energy nucleus-nucleus collisions were recorded using the PHENIX detector at the Relativistic Heavy Ion Collider (RHIC). The comprehensive set of measurements from the first three years of RHIC operation includes charged particle multiplicities, transverse energy, yield ratios and spectra of identified hadrons in a wide range of transverse momenta (p_T), elliptic flow, two-particle correlations, non-statistical fluctuations, and suppression of particle production at high p_T. The results are examined with an emphasis on implications for the formation of a new state of dense matter. We find that the state of matter created at RHIC cannot be described in terms of ordinary color neutral hadrons.Comment: 510 authors, 127 pages text, 56 figures, 1 tables, LaTeX. Submitted to Nuclear Physics A as a regular article; v3 has minor changes in response to referee comments. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.htm

    Interactions between donor age and 12-month estimated glomerular filtration rate on allograft and patient outcomes after kidney transplantation

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    Reduced estimated glomerular filtration rate (eGFR) at 12-months after kidney transplantation is associated with increased risk of allograft loss, but it is uncertain whether donor age and types modify this relationship. Using Australia and New Zealand registry data, multivariable Cox proportional modelling was used to examine the interactive effects between donor age, types and 12-month eGFR on overall allograft loss. We included 11,095 recipients (4,423 received live-donors). Recipients with lowest 12-month eGFR (60 ml/min/1.73 mÂČ) was 0.67 [0.62–0.74]. The association of 12-month eGFR and allograft loss was modified by donor age (but not donor types) where a higher risk of allograft loss in recipients with lower compared with higher 12-month eGFR being most pronounced in the younger donor age groups (p 60 ml/min/1.73 mÂČ, and the magnitude of the increased risk is most marked among recipients with younger donors. Careful deliberation of other factors including donor age when considering eGFR as a surrogate for clinical endpoints is warranted.Wai H. Lim, Esther Ooi, Helen L. Pilmore, David W. Johnson, Stephen P. McDonald, Philip Clayton, Carmel Hawley, William R. Mulley, Ross Francis, Michael G. Collins, Bryon Jaques, Nicholas G. Larkins, Christopher E. Davies, Kate Wyburn, Steve J. Chadban and Germaine Won

    Measurement of Transverse Single-Spin Asymmetries for Mid-rapidity Production of Neutral Pions and Charged Hadrons in Polarized p+p Collisions at sqrt(s) = 200 GeV

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    The transverse single-spin asymmetries of neutral pions and non-identified charged hadrons have been measured at mid-rapidity in polarized proton-proton collisions at sqrt(s) = 200 GeV. The data cover a transverse momentum (p_T) range 0.5-5.0 GeV/c for charged hadrons and 1.0-5.0 GeV/c for neutral pions, at a Feynman-x (x_F) value of approximately zero. The asymmetries seen in this previously unexplored kinematic region are consistent with zero within statistical errors of a few percent. In addition, the inclusive charged hadron cross section at mid-rapidity from 0.5 < p_T < 7.0 GeV/c is presented and compared to NLO pQCD calculations. Successful description of the unpolarized cross section above ~2 GeV/c using NLO pQCD suggests that pQCD is applicable in the interpretation of the asymmetry results in the relevant kinematic range.Comment: 331 authors, 6 pages text, 2 figures, 3 tables. Submitted to Phys. Rev. Lett. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.htm

    Measurement of the polarisation of W bosons produced with large transverse momentum in pp collisions at sqrt(s) = 7 TeV with the ATLAS experiment

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    This paper describes an analysis of the angular distribution of W->enu and W->munu decays, using data from pp collisions at sqrt(s) = 7 TeV recorded with the ATLAS detector at the LHC in 2010, corresponding to an integrated luminosity of about 35 pb^-1. Using the decay lepton transverse momentum and the missing transverse energy, the W decay angular distribution projected onto the transverse plane is obtained and analysed in terms of helicity fractions f0, fL and fR over two ranges of W transverse momentum (ptw): 35 < ptw < 50 GeV and ptw > 50 GeV. Good agreement is found with theoretical predictions. For ptw > 50 GeV, the values of f0 and fL-fR, averaged over charge and lepton flavour, are measured to be : f0 = 0.127 +/- 0.030 +/- 0.108 and fL-fR = 0.252 +/- 0.017 +/- 0.030, where the first uncertainties are statistical, and the second include all systematic effects.Comment: 19 pages plus author list (34 pages total), 9 figures, 11 tables, revised author list, matches European Journal of Physics C versio
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